Photonics Research, Volume. 3, Issue 2, A25(2015)
Nanosecond-pulsed, dual-wavelength, passively Q-switched ytterbium-doped bulk laser based on few-layer MoS2 saturable absorber
[1] [1] T. Hasan, Z. Sun, F. Wang, F. Bonaccorso, P. H. Tan, A. G. Rozhin, and A. C. Ferrari, “Nanotube-polymer composites for ultrafast photonics,” Adv. Mater. 21, 3874–3899 (2009).
[2] [2] Q. L. Bao, H. Zhang, Y. Wang, Z. H. Ni, Y. L. Yan, Z. X. Shen, K. P. Loh, and D. Y. Tang, “Atomic layer graphene as saturable absorber for ultrafast pulsed laser,” Adv. Funct. Mater. 19, 3077–3083 (2009).
[3] [3] A. Martinez, K. Fuse, and S. Yamashita, “Mechanical exfoliation of graphene for the passive mode-locking of fiber lasers,” Appl. Phys. Lett. 99, 121107 (2011).
[4] [4] H. Zhang, Q. L. Bao, D. Y. Tang, L. M. Zhao, and K. P. Loh, “Large energy soliton erbium-doped fiber laser with a graphene-polymer composite mode locker,” Appl. Phys. Lett. 95, 141103 (2009).
[5] [5] I. H. Baek, H. W. Lee, S. Bae, B. H. Hong, Y. H. Ahn, D. Yeom, and F. Rotermund, “Efficient mode-locking of sub-70-fs Ti:sapphire laser by graphene saturable absorber,” Appl. Phys. Express 5, 032701 (2012).
[6] [6] F. Lou, L. Cui, Y. B. Li, J. Hou, J. L. He, Z. T. Jia, J. Q. Liu, B. T. Zhang, K. J. Yang, Z. W. Wang, and X. T. Tao, “High-efficiency femtosecond Yb:Gd3Al0.5Ga4.5O12 mode-locked laser based on reduced graphene oxide,” Opt. Lett. 38, 4189–4192 (2013).
[7] [7] J. L. Xu, X. L. Li, J. L. He, X. P. Hao, Y. Z. Wu, Y. Yang, and K. J. Yang, “Performance of large-area few-layer graphene saturable absorber in femtosecond bulk laser,” Appl. Phys. Lett. 99, 261107 (2011).
[8] [8] E. Ugolotti, A. Schmidt, V. Petrov, J. W. Kim, D. Yeom, F. Rotermund, S. Bae, B. H. Hong, A. Agnesi, C. Fiebig, G. Erbert, X. Mateos, M. Aguiló, F. Diaz, and U. Griebner, “Graphene mode-locked femtosecond Yb:KLuW laser,” Appl. Phys. Lett. 101, 161112 (2012).
[9] [9] J. Ma, G. Q. Xie, P. Lv, W. L. Gao, P. Yuan, L. J. Qian, H. H. Yu, H. J. Zhang, J. Y. Wang, and D. Y. Tang, “Graphene mode-locked femtosecond laser at 2 μm wavelength,” Opt. Lett. 37, 2085–2087 (2012).
[10] [10] M. N. Cizmeciyan, J. W. Kim, S. Bae, B. H. Hong, F. Rotermund, and A. Sennaroglu, “Graphene mode-locked femtosecond Cr:ZnSe laser at 2500 nm,” Opt. Lett. 38, 341–343 (2013).
[11] [11] J. Liu, Y. G. Wang, Z. S. Qu, L. H. Zheng, L. B. Su, and J. Xu, “Graphene oxide absorber for 2 μm passive mode-locking Tm:YAlO3 laser,” Laser Phys. Lett. 9, 15–19 (2012).
[12] [12] S. Han, X. Li, H. Xu, Y. Zhao, H. Yu, H. Zhang, Y. Wu, Z. Wang, X. Hao, and X. Xu, “Graphene Q-switched 0.9-μm Nd:La0.11Y0.89VO4 laser,” Chin. Opt. Lett. 12, 011401 (2014).
[13] [13] X. L. Li, J. L. Xu, Y. Z. Wu, J. L. He, and X. P. Hao, “Large energy laser pulses with high repetition rate by graphene Q-switched solid-state laser,” Opt. Express 19, 9951–9955 (2011).
[14] [14] J. L. Xu, X. L. Li, J. L. He, X. P. Hao, Y. Yang, Y. Z. Wu, S. D. Liu, and B. T. Zhang, “Efficient graphene Q-switching and mode locking of 1.34 μm neodymium lasers,” Opt. Lett. 37, 2652– 2654 (2012).
[15] [15] Z. X. Zhu, Y. Wang, H. Chen, H. T. Huang, D. Y. Shen, J. Zhang, and D. Y. Tang, “A graphene-based passively Q-switched polycrystalline Er:YAG ceramic laser operation at 1645 nm,” Laser Phys. Lett. 10, 055801 (2013).
[16] [16] J. Hou, B. T. Zhang, J. L. He, Z. W. Wang, F. Lou, J. Ning, R. W. Zhao, and X. C. Su, “Passively Q-switched 2 μm Tm:YAP laser based on graphene saturable absorber mirror,” Appl. Opt. 53, 4968–4971 (2014).
[17] [17] M. Z. Hasan and C. L. Kane, “Colloquium: topological insulators,” Rev. Mod. Phys. 82, 3045–3067 (2010).
[18] [18] X. L. Qi and S. C. Zhang, “Topological insulators and superconductors,” Rev. Mod. Phys. 83, 1057–1110 (2011).
[19] [19] H. Yu, H. Zhang, Y. Wang, C. Zhao, B. Wang, S. Wen, H. Zhang, and J. Wang, “Topological insulator as an optical modulator for pulsed solid-state lasers,” Laser Photon. Rev. 7, L77–L83 (2013).
[20] [20] P. Tang, X. Zhang, C. Zhao, Y. Wang, H. Zhang, D. Shen, S. Wen, D. Tang, and D. Fan, “Topological insulator Bi2Te3 saturable for the passive Q-switching operation of an in-band pumped 1645- nm Er:YAG ceramic laser,” IEEE Photon. J. 5, 1500707 (2013).
[21] [21] F. Q. Jia, H. Chen, P. Liu, Y. Z. Huang, and Z. Q. Luo, “Nanosecond-pulsed, dual-wavelength passively Q-switched c-cut Nd:YVO4 laser using a few-layer Bi2Se3 saturable absorber,” IEEE J. Sel. Top. Quantum Electron.
[22] [22] 1601806 (2015). 22. C. Zhao, Y. Zou, Y. Chen, Z. Wang, S. Lu, H. Zhang, S. Wen, and D. Tang, “Wavelength-tunable picosecond soliton fiber laser with topological insulator: Bi2Se3 as a mode locker,” Opt. Express 20, 27888–27895 (2012).
[23] [23] Y. Chen, C. Zhao, H. Huang, S. Chen, P. Tang, Z. Wang, S. Lu, H. Zhang, S. Wen, and D. Tang, “Self-assembled topological insulator: Bi2Se3 membrane as a passive Q-switcher in an erbiumdoped fiber laser,” J. Lightwave Technol. 31, 2857–2863 (2013).
[24] [24] C. Zhao, H. Zhang, X. Qi, Y. Chen, Z. Wang, S. Wen, and D. Tang, “Ultra-short pulse generation by a topological insulator based saturable absorber,” Appl. Phys. Lett. 101, 211106 (2012).
[25] [25] Z. Q. Luo, Y. Z. Huang, J. Weng, H. H. Cheng, Z. Q. Lin, B. Xu, Z. P. Cai, and H. Y. Xu, “1.06 μm Q-switched ytterbium-doped fiber laser using few-layer topological insulator Bi2Se3 as a saturable absorber,” Opt. Express 21, 29516–29522 (2013).
[26] [26] Y. L. Li, Y. Rao, K. F. Mak, Y. M. You, S. Y. Wang, C. R. Dean, and T. F. Heinz, “Probing symmetry properties of few-layer MoS2 and h-BN by optical second-harmonic generation,” Nano Lett. 13, 3329–3333 (2013).
[27] [27] R. Wang, H. C. Chien, J. Kumar, N. Kumar, H. Y. Chiu, and H. Zhao, “Third-harmonic generation in ultrathin films of MoS2,” ACS Appl. Mater. Interface 6, 314–318 (2014).
[28] [28] W. T. Hsu, Z. A. Zhao, L. J. Li, C. H. Chen, M. H. Chiu, P. S. Chang, Y. C. Chou, and W. H. Chang, “Second harmonic generation from artificially stacked transition metal dichalcogenide twisted bilayers,” ACS Nano 8, 2951–2958 (2014).
[29] [29] K. P. Wang, J. Wang, J. T. Fan, M. Lotya, A. O’Neill, D. Fox, Y. Y. Feng, X. Y. Zhang, B. X. Jiang, Q. Z. Zhao, H. Z. Zhang, J. N. Coleman, L. Zhang, and W. Josef, “Ultrafast saturable absorption of two-dimensional MoS2 nanosheets,” ACS Nano 7, 9260–9267 (2013).
[30] [30] S. X. Wang, H. H. Yu, H. J. Zhang, A. Z. Wang, M. W. Zhao, Y. X. Chen, L. M. Mei, and J. Y. Wang, “Broadband few-layer MoS2 saturable absorbers,” Adv. Mater. 26, 3538–3544 (2014).
[31] [31] J. Du, Q. K. Wang, G. B. Jiang, C. W. Xu, C. J. Zhao, Y. J. Xiang, Y. Chen, S. C. Wen, and H. Zhang, “Ytterbium-doped fiber laser passively mode locked by few-layer molybdenum disulfide (MoS2) saturable absorber functioned with evanescent field,” Sci. Rep. 4, 6346 (2014).
[32] [32] H. Zhang, S. B. Lu, J. Zheng, J. Du, S. C. Wen, D. Y. Tang, and K. P. Loh, “Molybdenum disulfide (MoS2) as a broadband saturable absorber for ultra-fast photonics,” Opt. Express 22, 7249–7260 (2014).
[33] [33] H. D. Xia, H. P. Li, C. Y. Lan, C. Li, X. X. Zhang, S. J. Zhang, and Y. Liu, “Ultrafast erbium-doped fiber laser mode-locked by a CVDgrown molybdenum disulfide (MoS2) saturable absorber,” Opt. Express 22, 17341–17348 (2014).
[34] [34] H. Liu, A. P. Luo, F. Z. Wang, R. Tang, M. Liu, Z. C. Luo, W. C. Xu, C. J. Zhao, and H. Zhang, “Femtosecond pulse erbium-doped fiber laser by a few-layer MoS2 saturable absorber,” Opt. Lett. 39, 4591–4594 (2014).
[35] [35] B. Xu, Y. J. Cheng, Y. Wang, Y. Z. Huang, J. Peng, Z. Q. Luo, H. Y. Xu, Z. P. Cai, J. Weng, and R. Moncorgé, “Passively Q-switched Nd:YAlO3 nanosecond laser using MoS2 as saturable absorber,” Opt. Express 22, 28934–28940 (2014).
[36] [36] Z. Q. Luo, Y. Z. Huang, M. Zhong, Y. Y. Li, J. Y. Wu, B. Xu, H. Y. Xu, Z. P. Cai, J. Peng, and J. Weng, “1-, 1.5-, and 2-μm fiber lasers Q-switched by a broadband few-layer MoS2 saturable absorber,” J. Lightwave Technol. 32, 4077–4084 (2014).
[37] [37] S. Bertolazzi, J. Brivio, and A. Kis, “Stretching and breaking of ultrathin MoS2,” ACS Nano 5, 9703–9709 (2011).
[38] [38] B. Radisavljevic, A. Radenovic, J. Brivio, V. Giacometti, and A. Kis, “Single-layer MoS2 transistors,” Nat. Nanotechnol. 6, 147–150 (2011).
[39] [39] H. Li, Q. Zhang, C. C. R. Yap, B. K. Tay, T. H. Edwin, A. Olivier, and D. Baillargeat, “From bulk to monolayer MoS2: evolution of Raman scattering,” Adv. Funct. Mater. 22, 1385–1390 (2012).
[40] [40] T. Li and G. Galli, “Electronic properties of MoS2 nanoparticles,” J. Phys. Chem. C 111, 16192–16196 (2007).
[41] [41] Z. C. Luo, M. Liu, H. Liu, X. W. Zheng, A. P. Luo, C. J. Zhao, H. Zhang, S. C. Wen, and W. C. Xu, “2 GHz passively harmonic mode-locked fiber laser by a microfiber-based topological insulator saturable absorber,” Opt. Lett. 38, 5212–5215 (2013).
[42] [42] F. Lou, Z. T. Jia, J. L. He, R. W. Zhao, J. Hou, Z. W. Wang, S. D. Liu, B. T. Zhang, and C. M. Dong, “Efficient high-peak power wavelength-switchable femtosecond Yb:LGGG laser,” IEEE Photon. Technol. Lett. 27, 407–410 (2015).
[43] [43] S. Sahoo, A. P. S. Gaur, M. Ahmadi, M. J.-F. Guinel, and R. S. Katiyar, “Temperature-dependent Raman studies and thermal conductivity of few-layer MoS2,” J. Phys. Chem. C 117, 9042– 9047 (2013).
[44] [44] W. Li, J. Carrete, and N. Mingo, “Thermal conductivity and phonon linewidths of monolayer MoS2 from first principles,” Appl. Phys. Lett. 103, 253103 (2013).
Get Citation
Copy Citation Text
Fei Lou, Ruwei Zhao, Jingliang He, Zhitai Jia, Xiancui Su, Zhaowei Wang, Jia Hou, Baitao Zhang, "Nanosecond-pulsed, dual-wavelength, passively Q-switched ytterbium-doped bulk laser based on few-layer MoS2 saturable absorber," Photonics Res. 3, A25 (2015)
Special Issue: PHOTONICS BASED ON TWO DIMENSIONAL MATERIALS
Received: Nov. 14, 2014
Accepted: Jan. 7, 2015
Published Online: Jan. 6, 2016
The Author Email: Jingliang He (jlhe@sdu.edu.cn)